In Fig.3 we show the parameter space in the two-parameter plane of \(m_S\)  and \(A_{\lambda }\) ,
for \(\lambda =1.2\)  and \(\tan \beta =\lbrace 4.5, 5, 5.5\rbrace \) , respectively.
For each \(\tan \beta \)  region below the color contour is excluded by the condition of stability of potential
and mass bound on chargino mass \(m_{\chi }>103\)  GeV [1]}.
Region in the right up corner is excluded by the precision measurement of Higgs coupling presently.
In particular, \(m_{S}\)  heavier than \(\sim \) 90, 105, and 110 GeV is excluded for \(\tan \beta =4.5\) , 5 and 5.5, respectively.
In comparison with the choice \(\lambda =0.7\)  discussed in [2]},
the main difference is that for \(\lambda =1.2\)  it allows larger \(m_{S}\) .
